{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.145862.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2773780"}},{"@id":"https://doi.org/10.1007/JHEP10(2024)209","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2024","description":"Diboson production in association with jets is studied in the fully leptonic final states, $\\textrm{pp} \\to (\\textrm{Z}/\\gamma^*)(\\textrm{Z}/\\gamma^*)+\\textrm{jets} \\to 2\\ell2\\ell'+\\textrm{jets}$, ($\\ell,\\ell' = \\textrm{e}$ or $\\mu$) in proton-proton collisions at a center-of-mass energy of 13 TeV. The data sample corresponds to an integrated luminosity of 138 fb$^{-1}$ collected with the CMS detector at the LHC. Differential distributions and normalized differential cross sections are measured as a function of jet multiplicity, transverse momentum $p_\\textrm{T}$, pseudorapidity $\\eta$, invariant mass and $\\Delta\\eta$ of the highest-$p_\\textrm{T}$ and second-highest-$p_\\textrm{T}$ jets, and as a function of invariant mass of the four-lepton system for events with various jet multiplicities. These differential cross sections are compared with theoretical predictions that mostly agree with the experimental data. However, in a few regions we observe discrepancies between the predicted and measured values. Further improvement of the predictions is required to describe the ZZ+jets production in the whole phase space.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.145862.v1/t1","@type":"Dataset","description":"Differential cross sections normalized to the fiducial cross section as a function of the invariant mass of the four-lepton system,...","name":"Figure 7 (left)"},{"@id":"https://doi.org/10.17182/hepdata.145862.v1/t2","@type":"Dataset","description":"Differential cross sections normalized to the fiducial cross section as a function of the number of jets with $p_T >...","name":"Figure 7 (right)"},{"@id":"https://doi.org/10.17182/hepdata.145862.v1/t3","@type":"Dataset","description":"Differential cross sections normalized to the fiducial cross section as a function of the $p_T$ of the highest-$p_T$ jet","name":"Figure 8 (upper left)"},{"@id":"https://doi.org/10.17182/hepdata.145862.v1/t4","@type":"Dataset","description":"Differential cross sections normalized to the fiducial cross section as a function of the $p_T$ of the second-highest-$p_T$ jet","name":"Figure 8 (upper right)"},{"@id":"https://doi.org/10.17182/hepdata.145862.v1/t5","@type":"Dataset","description":"Differential cross sections normalized to the fiducial cross section as a function of the $|\\eta|$ of the highest-$p_T$ jet","name":"Figure 8 (lower left)"},{"@id":"https://doi.org/10.17182/hepdata.145862.v1/t6","@type":"Dataset","description":"Differential cross sections normalized to the fiducial cross section as a function of the $|\\eta|$ of the second-highest-$p_T$ jet","name":"Figure 8 (lower right)"},{"@id":"https://doi.org/10.17182/hepdata.145862.v1/t7","@type":"Dataset","description":"Differential cross sections normalized to the fiducial cross section as a function of the pseudorapidity difference between the two highest-$p_T$...","name":"Figure 9 (left)"},{"@id":"https://doi.org/10.17182/hepdata.145862.v1/t8","@type":"Dataset","description":"Differential cross sections normalized to the fiducial cross section as a function of the invariant mass of the two highest-$p_T$...","name":"Figure 9 (right)"},{"@id":"https://doi.org/10.17182/hepdata.145862.v1/t9","@type":"Dataset","description":"Differential cross sections normalized to the fiducial cross section as a function of the invariant mass of the four-lepton system,...","name":"Figure 10"},{"@id":"https://doi.org/10.17182/hepdata.145862.v1/t10","@type":"Dataset","description":"Differential cross sections normalized to the fiducial cross section as a function of the invariant mass of the four-lepton system...","name":"Figure 11 (upper left)."},{"@id":"https://doi.org/10.17182/hepdata.145862.v1/t11","@type":"Dataset","description":"Differential cross sections normalized to the fiducial cross section as a function of the invariant mass of the four-lepton system...","name":"Figure 11 (upper right)."},{"@id":"https://doi.org/10.17182/hepdata.145862.v1/t12","@type":"Dataset","description":"Differential cross sections normalized to the fiducial cross section as a function of the invariant mass of the four-lepton system...","name":"Figure 11 (lower left)."},{"@id":"https://doi.org/10.17182/hepdata.145862.v1/t13","@type":"Dataset","description":"Differential cross sections normalized to the fiducial cross section as a function of the invariant mass of the four-lepton system...","name":"Figure 11 (lower right)."},{"@id":"https://doi.org/10.17182/hepdata.145862.v1/t14","@type":"Dataset","description":"Differential cross sections normalized to the fiducial cross section as a function of the invariant mass of the four-lepton system...","name":"Figure 12 (upper left)."},{"@id":"https://doi.org/10.17182/hepdata.145862.v1/t15","@type":"Dataset","description":"Differential cross sections normalized to the fiducial cross section as a function of the invariant mass of the four-lepton system...","name":"Figure 12 (upper right)."},{"@id":"https://doi.org/10.17182/hepdata.145862.v1/t16","@type":"Dataset","description":"Differential cross sections normalized to the fiducial cross section as a function of the invariant mass of the four-lepton system...","name":"Figure 12 (lower left)."},{"@id":"https://doi.org/10.17182/hepdata.145862.v1/t17","@type":"Dataset","description":"Differential cross sections normalized to the fiducial cross section as a function of the invariant mass of the four-lepton system...","name":"Figure 12 (lower right)."}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2773780?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/145862"}],"inLanguage":"en","name":"Measurement of differential ZZ + jets production cross sections in pp collisions at $\\sqrt{s}$ = 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2773780?version=1","version":1}